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Factoring the strong CP problem
by
Agrawal, Prateek
, Howe, Kiel
in
Anomalies in Field and String Theories
/ Beyond Standard Model
/ Classical and Quantum Gravitation
/ CP violation
/ Elementary Particles
/ Fermions
/ High energy physics
/ Physics
/ Physics and Astronomy
/ PHYSICS OF ELEMENTARY PARTICLES AND FIELDS
/ Quantum Field Theories
/ Quantum Field Theory
/ Quantum Physics
/ Regular Article - Theoretical Physics
/ Relativity Theory
/ Solitons Monopoles and Instantons
/ String Theory
/ Subgroups
2018
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Factoring the strong CP problem
by
Agrawal, Prateek
, Howe, Kiel
in
Anomalies in Field and String Theories
/ Beyond Standard Model
/ Classical and Quantum Gravitation
/ CP violation
/ Elementary Particles
/ Fermions
/ High energy physics
/ Physics
/ Physics and Astronomy
/ PHYSICS OF ELEMENTARY PARTICLES AND FIELDS
/ Quantum Field Theories
/ Quantum Field Theory
/ Quantum Physics
/ Regular Article - Theoretical Physics
/ Relativity Theory
/ Solitons Monopoles and Instantons
/ String Theory
/ Subgroups
2018
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Do you wish to request the book?
Factoring the strong CP problem
by
Agrawal, Prateek
, Howe, Kiel
in
Anomalies in Field and String Theories
/ Beyond Standard Model
/ Classical and Quantum Gravitation
/ CP violation
/ Elementary Particles
/ Fermions
/ High energy physics
/ Physics
/ Physics and Astronomy
/ PHYSICS OF ELEMENTARY PARTICLES AND FIELDS
/ Quantum Field Theories
/ Quantum Field Theory
/ Quantum Physics
/ Regular Article - Theoretical Physics
/ Relativity Theory
/ Solitons Monopoles and Instantons
/ String Theory
/ Subgroups
2018
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Journal Article
Factoring the strong CP problem
2018
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Overview
A
bstract
We present a new mechanism to solve the strong CP problem using
N
≥ 2 axions, each dynamically relaxing part of the θ parameter. At high energies
M
≫ Λ
QCD
the SU(3)
c
group becomes the diagonal subgroup of an SU(3)
N
gauge group, and the non-perturbative effects in each individual SU(3) factor generate a potential for the corresponding axion. The vacuum is naturally aligned to ensure
θ
¯
=
0
at low energies, and the masses of these axions can be much larger than for the standard QCD axion. This mechanism avoids the introduction of a discrete Z
2
symmetry and associated ‘mirror’ copies of the SM fermions, and also avoids the introduction and stabilization of new light colored states to modify the running of the QCD gauge coupling found in other heavy axion models. This strengthens the motivation for axion-like particles solving the strong CP problem at points beyond the standard QCD axion curve in the (
m
a
,
f
a
) plane.
Publisher
Springer Berlin Heidelberg,Springer Nature B.V,Springer Berlin,SpringerOpen
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